Measurement-induced steering of quantum systems

TL;DR

This paper presents a general protocol for steering quantum systems towards desired states by coupling them with auxiliary qubits and using measurement-induced back-action, applicable to both few-body and many-body systems.

Contribution

It introduces a novel, general framework for quantum state steering via repeated system-detector interactions and measurements, with practical implementation considerations.

Findings

Successfully steered a pair of spins-1/2 to the singlet state.

Steered a spin-1 chain to the AKLT state.

Protocols are compatible with current quantum technology.

Abstract

We set out a general protocol for steering the state of a quantum system from an arbitrary initial state towards a chosen target state by coupling it to auxiliary quantum degrees of freedom. The protocol requires multiple repetitions of an elementary step: during each step the system evolves for a fixed time while coupled to auxiliary degrees of freedom (which we term 'detector qubits') that have been prepared in a specified initial state. The detectors are discarded at the end of the step, or equivalently, their state is determined by a projective measurement with an unbiased average over all outcomes. The steering harnesses back-action of the detector qubits on the system, arising from entanglement generated during the coupled evolution. We establish principles for the design of the system-detector coupling that ensure steering of a desired form. We illustrate our general ideas using both few-body examples (including a pair of spins-1/2 steered to the singlet state) and a many-body example (a spin-1 chain steered to the Affleck-Kennedy-Lieb-Tasaki state). We study the continuous time limit in our approach and discuss similarities to (and differences from) drive-and-dissipation protocols for quantum state engineering. Our protocols are amenable to implementations using present-day technology. Obvious extensions of our analysis include engineering of other many-body phases in one and higher spatial dimensions, adiabatic manipulations of the target states, and the incorporation of active error correction steps.